功能材料
功能材料
공능재료
JOURNAL OF FUNCTIONAL MATERIALS
2014年
12期
12070-12073,12078
,共5页
杨中服%胡义华%陈丽%王小涓
楊中服%鬍義華%陳麗%王小涓
양중복%호의화%진려%왕소연
长余辉%Ba4(Si3O8)2%Nd3+%二阶动力学
長餘輝%Ba4(Si3O8)2%Nd3+%二階動力學
장여휘%Ba4(Si3O8)2%Nd3+%이계동역학
long afterglow%Ba4(Si3O8)2%Nd3+%kinetics order
使用高温固相法合成了长余辉发光材料Ba3.88-x(Si3O8)2∶0.12Eu2+,xNd3+。实验分别获得了样品的晶体结构、激发与发射谱、余辉衰减、热释光等信息。样品呈现 Eu2+的宽带发射,发射峰位在495 nm,Nd3+的共掺没有引入新的发光中心;Nd3+共掺对材料的荧光强度和余辉强度都有明显的提高,并延长了余辉时间,Nd3+共掺的最优比例为 x=0.04,此条件下材料的肉眼可视的余辉时间从 Eu2+单掺的约20 min延长至1 h;通过对样品的不同等待时间的热释光分析,发现热释光峰位随时间向高温方向移动,过程中半高宽基本不变,对称因子μg 维持在0.52左右,对应的陷阱深度为0.89 eV,陷阱释放载流子的过程可视为二阶动力学过程。
使用高溫固相法閤成瞭長餘輝髮光材料Ba3.88-x(Si3O8)2∶0.12Eu2+,xNd3+。實驗分彆穫得瞭樣品的晶體結構、激髮與髮射譜、餘輝衰減、熱釋光等信息。樣品呈現 Eu2+的寬帶髮射,髮射峰位在495 nm,Nd3+的共摻沒有引入新的髮光中心;Nd3+共摻對材料的熒光彊度和餘輝彊度都有明顯的提高,併延長瞭餘輝時間,Nd3+共摻的最優比例為 x=0.04,此條件下材料的肉眼可視的餘輝時間從 Eu2+單摻的約20 min延長至1 h;通過對樣品的不同等待時間的熱釋光分析,髮現熱釋光峰位隨時間嚮高溫方嚮移動,過程中半高寬基本不變,對稱因子μg 維持在0.52左右,對應的陷阱深度為0.89 eV,陷阱釋放載流子的過程可視為二階動力學過程。
사용고온고상법합성료장여휘발광재료Ba3.88-x(Si3O8)2∶0.12Eu2+,xNd3+。실험분별획득료양품적정체결구、격발여발사보、여휘쇠감、열석광등신식。양품정현 Eu2+적관대발사,발사봉위재495 nm,Nd3+적공참몰유인입신적발광중심;Nd3+공참대재료적형광강도화여휘강도도유명현적제고,병연장료여휘시간,Nd3+공참적최우비례위 x=0.04,차조건하재료적육안가시적여휘시간종 Eu2+단참적약20 min연장지1 h;통과대양품적불동등대시간적열석광분석,발현열석광봉위수시간향고온방향이동,과정중반고관기본불변,대칭인자μg 유지재0.52좌우,대응적함정심도위0.89 eV,함정석방재류자적과정가시위이계동역학과정。
Long afterglow phosphors Ba3.88-x(Si3O8)2∶0.12Eu2+,xNd3+ were synthesized by a solid state reac-tion.The crystal structure,excitation spectra,emission spectra,long afterglow decaying curves and thermolu-minescence (TL)curves of samples were obtained in our work.The samples show a broad emission band of Eu2+ centered at 495 nm,and no new luminescent center appeared with Nd3+ co-doping.The fluorescence and afterglow intensities were both magnified obviously with Nd3+ co-doping,and the afterglow time prolonged. The optimal proportion of Nd2+ single doping was x=0.12,exhibiting a long-lasting phosphorescence lasting for 1 h visible to the naked eyes,more than 20 min with Eu2+ single doped.The analysis of TL with different waiting time shown that the TL peak shifts to the higher temperature with time prolongs,the half widths re-main unchanged,the symmetry constantμg was about 0.52,the traps depth was 0.89 eV,and the process of releasing carriers was very close to the second order kinetics.